EP3308180A1 - Method and apparatus for identifying sensitive integrated circuit parts to random telegraph signal - Google Patents
Method and apparatus for identifying sensitive integrated circuit parts to random telegraph signalInfo
- Publication number
- EP3308180A1 EP3308180A1 EP16730301.5A EP16730301A EP3308180A1 EP 3308180 A1 EP3308180 A1 EP 3308180A1 EP 16730301 A EP16730301 A EP 16730301A EP 3308180 A1 EP3308180 A1 EP 3308180A1
- Authority
- EP
- European Patent Office
- Prior art keywords
- integrated circuit
- scan area
- rts
- rts noise
- response
- Prior art date
- Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
- Withdrawn
Links
Classifications
-
- H—ELECTRICITY
- H04—ELECTRIC COMMUNICATION TECHNIQUE
- H04W—WIRELESS COMMUNICATION NETWORKS
- H04W52/00—Power management, e.g. Transmission Power Control [TPC] or power classes
- H04W52/04—Transmission power control [TPC]
- H04W52/30—Transmission power control [TPC] using constraints in the total amount of available transmission power
- H04W52/36—Transmission power control [TPC] using constraints in the total amount of available transmission power with a discrete range or set of values, e.g. step size, ramping or offsets
- H04W52/367—Power values between minimum and maximum limits, e.g. dynamic range
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01R—MEASURING ELECTRIC VARIABLES; MEASURING MAGNETIC VARIABLES
- G01R31/00—Arrangements for testing electric properties; Arrangements for locating electric faults; Arrangements for electrical testing characterised by what is being tested not provided for elsewhere
- G01R31/28—Testing of electronic circuits, e.g. by signal tracer
- G01R31/302—Contactless testing
- G01R31/308—Contactless testing using non-ionising electromagnetic radiation, e.g. optical radiation
- G01R31/311—Contactless testing using non-ionising electromagnetic radiation, e.g. optical radiation of integrated circuits
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01R—MEASURING ELECTRIC VARIABLES; MEASURING MAGNETIC VARIABLES
- G01R31/00—Arrangements for testing electric properties; Arrangements for locating electric faults; Arrangements for electrical testing characterised by what is being tested not provided for elsewhere
- G01R31/26—Testing of individual semiconductor devices
- G01R31/2607—Circuits therefor
- G01R31/2621—Circuits therefor for testing field effect transistors, i.e. FET's
- G01R31/2626—Circuits therefor for testing field effect transistors, i.e. FET's for measuring noise
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01R—MEASURING ELECTRIC VARIABLES; MEASURING MAGNETIC VARIABLES
- G01R31/00—Arrangements for testing electric properties; Arrangements for locating electric faults; Arrangements for electrical testing characterised by what is being tested not provided for elsewhere
- G01R31/28—Testing of electronic circuits, e.g. by signal tracer
- G01R31/2851—Testing of integrated circuits [IC]
- G01R31/2855—Environmental, reliability or burn-in testing
- G01R31/2872—Environmental, reliability or burn-in testing related to electrical or environmental aspects, e.g. temperature, humidity, vibration, nuclear radiation
- G01R31/2874—Environmental, reliability or burn-in testing related to electrical or environmental aspects, e.g. temperature, humidity, vibration, nuclear radiation related to temperature
- G01R31/2875—Environmental, reliability or burn-in testing related to electrical or environmental aspects, e.g. temperature, humidity, vibration, nuclear radiation related to temperature related to heating
-
- H—ELECTRICITY
- H04—ELECTRIC COMMUNICATION TECHNIQUE
- H04W—WIRELESS COMMUNICATION NETWORKS
- H04W52/00—Power management, e.g. Transmission Power Control [TPC] or power classes
- H04W52/04—Transmission power control [TPC]
- H04W52/30—Transmission power control [TPC] using constraints in the total amount of available transmission power
- H04W52/32—TPC of broadcast or control channels
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01R—MEASURING ELECTRIC VARIABLES; MEASURING MAGNETIC VARIABLES
- G01R31/00—Arrangements for testing electric properties; Arrangements for locating electric faults; Arrangements for electrical testing characterised by what is being tested not provided for elsewhere
- G01R31/28—Testing of electronic circuits, e.g. by signal tracer
- G01R31/2832—Specific tests of electronic circuits not provided for elsewhere
- G01R31/2836—Fault-finding or characterising
- G01R31/2837—Characterising or performance testing, e.g. of frequency response
Definitions
- the present disclosure relates in general to testing and validation of electronic circuits, including without limitation methods and systems for identifying a semiconductor device or a portion thereof that exhibits low-frequency random telegraph signal (RTS) noise by local modification of such device's activation energy.
- RTS random telegraph signal
- RTS noise also known as burst noise, popcorn noise, impulse noise, and bi-stable noise
- MOSFET metal-oxide-semiconductor field-effect transistor
- RTS noise typically comprises sudden step-like transitions between two or more discrete current or voltage levels, often as high as several hundred microvolts, and often at random and unpredictable times.
- RTS noise may be created by the capture and emission of charge carriers and may result in two distinct states. Simulation models of RTS noise are not widely available, leading to the probability that a design with an unexpected sensitivity to RTS may be discovered after manufacturing of the semiconductor chip.
- Semiconductor dice with sensitive analog circuits or memories can exhibit a large RTS signature in a subset of the population of manufactured dice.
- one or more disadvantages and problems associated with existing approaches to identifying and measuring RTS noise may be reduced or eliminated.
- a method for identifying a location of an integrated circuit that is sensitive to RTS noise may include applying localized heat to a scan area of the integrated circuit, observing any change in one or more electrical parameters of the integrated circuit in response to the localized heat being applied to the scan area indicative of sensitivity to RTS noise, and identifying the location sensitive to RTS noise responsive to observing change in one or more electrical parameters of the integrated circuit indicative of sensitivity to RTS noise in response to the localized heat being applied to the scan area.
- a system for identifying a location of an integrated circuit that is sensitive to RTS noise may include a heat-generating device configured to apply localized heat to a scan area of the integrated circuit, RTS measurement equipment configured to observe any change in one or more electrical parameters of the integrated circuit indicative of sensitivity to RTS noise in response to the localized heat being applied to the scan area, and an RTS processing and system control configured to identify the location sensitive to RTS noise responsive to observing change in one or more electrical parameters of the integrated circuit indicative of sensitivity to RTS noise in response to the localized heat being applied to the scan area.
- FIGURE 1 illustrates a diagram of an example system for identification and measurement of RTS noise within a semiconductor device, in accordance with embodiments of the present disclosure
- FIGURES 2A-2C illustrate graphs depicting example measurements for an output of a resistor-capacitor oscillator versus time at three different temperatures, in accordance with embodiments of the present disclosure
- FIGURES 3A-3C illustrate graphs depicting example histograms of negative pulse probability for the frequency measurements depicted in FIGURES 2A-2C, in accordance with embodiments of the present disclosure.
- FIGURE 4 illustrates a flowchart of an example method for identification and measurement of RTS noise within a semiconductor device, in accordance with embodiments of the present disclosure.
- FIGURE 1 illustrates a diagram of an example system 100 for identification and measurement of RTS noise within a semiconductor device under test (DUT) 102, in accordance with embodiments of the present disclosure.
- DUT 102 may comprise a semiconductor die with one or more integrated circuits performed thereon.
- system 100 may include an RTS processing and system control module 104, a DUT configuration and test system 106, a laser control system 108, a laser 110, and RTS measurement equipment 112.
- Processing and system control module 104 may comprise any suitable system, device, or apparatus for controlling DUT configuration and test system 106, laser control system 108, and RTS measurement equipment 112, and/or configured to receive test information from RTS measurement equipment 112.
- Processing and system control module 104 may be embodied in hardware, software, firmware, or a combination thereof. Functionality of processing and system control module 104 is described in greater detail below.
- DUT configuration and test system 106 may comprise any suitable system, device, or apparatus for applying one or more test vectors of electronic stimuli to DUT 102 in order to perform analysis of DUT 102 in order to characterize operation of DUT 102, detect defects in DUT 102, and/or conduct other tests of DUT 102.
- DUT configuration and test system 106 may be controlled by processing and system control module 104.
- DUT configuration and test system 106 may be embodied in hardware, software, firmware, or a combination thereof.
- Laser control system 108 may comprise any suitable system, device, or apparatus for controlling an intensity, wavelength, and/or position of laser 110 with respect to DUT 102.
- Laser control system 108 may be embodied in hardware, software, firmware, or a combination thereof.
- Laser 110 may comprise any suitable system, device, or apparatus for generating a focused, collimated beam of photonic energy.
- laser 110 may also include a motor or other electromechanical apparatus under the control of laser control system 108 for translation in directions parallel to a surface of DUT 102, such that laser control system 108 may control a position of laser 110 in order to direct photonic energy of laser 110 to a specific location or locations (e.g., within scan area 114 shown in FIGURE 1) on DUT 102.
- laser 110 is selected to have a wavelength that will create a desired change in activation energy of fabricated components of DUT 102 (e.g., by applying localized heat), but will not otherwise significantly affect other electrical characteristics of DUT 102 (e.g., the selected wavelength will not cause significant generation of electron-hole pairs in the semiconductor substrate of DUT 102).
- scan area 114 is shown in FIGURE 1 as being a portion of DUT 102, in some embodiments, a scan area 114 may include the entirety of DUT 102.
- RTS measurement equipment 112 may comprise any suitable system, device, or apparatus for reading one or more selected electrical parameters generated from test vectors applied by DUT configuration and test system 106 in order to detect the presence of any RTS noise in DUT 102.
- electrical parameters that may be detected to indicate presence of RTS noise may include modulation of frequency in an oscillation circuit integral to DUT 102, modulation of an output signal of an amplifier integral to DUT 102, current modulation of a transistor or circuit integral to DUT 102, voltage modulation of a transistor or circuit integral to DUT 102, modulation of retention in a flash memory integral to DUT 102, random noise in an image sensor, and other electrical parameters.
- system 100 may identify and measure RTS noise by applying localized heat to a scan area 114 using laser 110 which may create a local change in activation energy (e.g., a decrease in activation energy) and by measuring changes in electrical parameters induced by such heat (e.g., with RTS measurement equipment 112), identify coordinates of DUT 102 in which RTS noise responds to changes in temperature.
- a local change in activation energy e.g., a decrease in activation energy
- RTS measurement equipment 112 e.g., a decrease in activation energy
- system 100 may enable an operator of system 100 to identify portions (e.g. one or more scan areas 114) in which one or more semiconductor structures (e.g., MOSFETs) which generate RTS noise are expected to be located.
- system 100 may cause laser 110 to move such that its beam "scans" across a scan area 114 to generate localized heating.
- Laser 110 may move in discrete steps or at a rate slow enough to allow the capture of an RTS measurement for each scan area 114.
- RTS measurement equipment 112 may measure electrical parameters (e.g., average pulse width for the observed RTS noise) for each scan area 114 until all scan areas 114 of DUT 102 have been fully tested.
- the location of a semiconductor structure (e.g., MOSFET) responsible for creating excessive RTS noise is determined by correlating the X,Y coordinates of laser 110 with a change in measured electrical parameters (e.g., a decrease in an observed average pulse width).
- RTS measurement equipment 112 may measure a pulse width of a resistive-capacitive oscillator to determine any presence of RTS noise.
- An average pulse width of RTS noise is a strong function of activation energy, and heating an area of semiconductor substrate including an integrated circuit exhibiting RTS noise is likely to lower such activation energy, thus resulting in a decrease in average pulse width associated with the RTS noise.
- FIGURES 2A-2C illustrate graphs depicting example measurements for an output of an RTS-noise generating resistor-capacitor oscillator versus time at three different temperatures (e.g., -15°C, 25°C, and 75°C), in accordance with embodiments of the present disclosure.
- RTS noise may cause the output of a resistive-capacitive oscillator to occasionally change frequency.
- RTS noise may be characterized by the average pulse width of these discrete changes in frequency.
- FIGURES 3A-3C illustrate graphs depicting example histograms of negative pulse probability from the measurements depicted in FIGURES 2A-2C, in accordance with embodiments of the present disclosure.
- FIGURES 3A-3C show that as heat is applied to a scan area 114 having structures that generate RTS noise, and the temperature of such scan area 114 is increased from -15°C to -25°C to 75°C (thus decreasing the activation energy for such scan area 114), the average pulse widths for RTS noise in such scan area 114 decreases at a logarithmic rate.
- a change e.g., decreasing pulse width with increasing temperature
- MOSFET e.g., MOSFET
- system 100 may observe a plurality of discrete noise levels, and measure such noise levels to determine a source of RTS noise.
- system 100 may analyze a multi-modal histogram (as shown in FIGURES 3A-3C) created by RTS noise.
- FIGURE 4 illustrates a flowchart of an example method 400 for identification and measurement of RTS noise within a semiconductor device, in accordance with embodiments of the present disclosure.
- method 400 may begin at step 402.
- teachings of the present disclosure may be implemented in a variety of configurations of system 100 as shown in FIGURE 1.
- the preferred initialization point for method 400 and the order of the steps comprising method 400 may depend on the implementation chosen.
- method 400 may be implemented as firmware, software, applications, functions, libraries, or other instructions.
- system 100 may measure electrical parameters induced by a particular test vector applied to DUT 102 (e.g., by DUT configuration and test system 106).
- system 100 may (e.g., using laser 110) apply heat to all or a large portion of DUT 102.
- system 100 may measure electrical parameters induced by the particular test vector. In some embodiments, steps 404 and 406 may be repeated at multiple temperatures.
- system 100 may determine if any changes have occurred to the measured electrical parameters as a result of application of the heat that indicate a presence of RTS noise. If changes have occurred to the measured electrical parameters as a result of application of the heat that indicate a presence of RTS noise, method 400 may proceed to step 410. Otherwise, method 400 may end.
- system 100 may identify one or more scan areas 114.
- system 100 may measure electrical parameters induced by a particular test vector applied to DUT 102 (e.g., by DUT configuration and test system 106).
- system 100 may (e.g., using laser 110) apply heat to such scan area 114.
- system 100 may measure electrical parameters induced by the particular test vector. In some embodiments, steps 414 and 416 may be repeated at multiple temperatures.
- system 100 may determine if any changes have occurred to the measured electrical parameters as a result of application of the heat that indicate a presence of RTS noise in the scan area 114.
- system 100 may determine if any scan areas 114 remain to be tested. If any scan areas 114 remain to be tested, steps 412 through 418 may be repeated for such scan areas 114 to identify which scan areas 114 exhibit characteristics of RTS noise. Otherwise, method 400 may end. In some embodiments, such identified scan areas 114 may be further analyzed (e.g., broken up into smaller scan areas with the heating and analysis steps described above repeated) in order to more precisely identify a location on DUT 102 which is a source of RTS noise.
- FIGURE 4 discloses a particular number of steps to be taken with respect to method 400, method 400 may be executed with greater or fewer steps than those depicted in FIGURE 4.
- FIGURE 4 discloses a certain order of steps to be taken with respect to method 400, the steps comprising method 400 may be completed in any suitable order.
- Method 400 may be implemented using system 100, components thereof, or any other system such as those shown in FIGURE 1 operable to implement method 400.
- method 400 may be implemented partially or fully in software and/or firmware embodied in computer-readable media.
- references in the appended claims to an apparatus or system or a component of an apparatus or system being adapted to, arranged to, capable of, configured to, enabled to, operable to, or operative to perform a particular function encompasses that apparatus, system, or component, whether or not it or that particular function is activated, turned on, or unlocked, as long as that apparatus, system, or component is so adapted, arranged, capable, configured, enabled, operable, or operative.
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- Engineering & Computer Science (AREA)
- Physics & Mathematics (AREA)
- General Physics & Mathematics (AREA)
- Microelectronics & Electronic Packaging (AREA)
- General Engineering & Computer Science (AREA)
- Health & Medical Sciences (AREA)
- Computer Hardware Design (AREA)
- Toxicology (AREA)
- Computer Vision & Pattern Recognition (AREA)
- Electromagnetism (AREA)
- Signal Processing (AREA)
- Computer Networks & Wireless Communication (AREA)
- Environmental & Geological Engineering (AREA)
- Testing Of Individual Semiconductor Devices (AREA)
- Investigating Or Analyzing Materials Using Thermal Means (AREA)
Abstract
Description
Claims
Applications Claiming Priority (3)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| US201562173075P | 2015-06-09 | 2015-06-09 | |
| US15/175,871 US9723578B2 (en) | 2015-06-09 | 2016-06-07 | Random telegraph signal identification and measurement |
| PCT/EP2016/063072 WO2016198475A1 (en) | 2015-06-09 | 2016-06-08 | Method and apparatus for identifying sensitive integrated circuit parts to random telegraph signal |
Publications (1)
| Publication Number | Publication Date |
|---|---|
| EP3308180A1 true EP3308180A1 (en) | 2018-04-18 |
Family
ID=56137291
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| EP16730301.5A Withdrawn EP3308180A1 (en) | 2015-06-09 | 2016-06-08 | Method and apparatus for identifying sensitive integrated circuit parts to random telegraph signal |
Country Status (5)
| Country | Link |
|---|---|
| US (1) | US9723578B2 (en) |
| EP (1) | EP3308180A1 (en) |
| KR (1) | KR102291679B1 (en) |
| CN (1) | CN107923940A (en) |
| WO (1) | WO2016198475A1 (en) |
Families Citing this family (3)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| KR102400557B1 (en) * | 2015-10-13 | 2022-05-20 | 삼성전자주식회사 | Circuit Design Method and Simulation Method considering random telegraph signal noise |
| CN110045193A (en) * | 2019-03-06 | 2019-07-23 | 珠海博雅科技有限公司 | A kind of floating-gate device thump telegraph repeater measuring system and measurement method |
| US11674995B2 (en) * | 2021-01-13 | 2023-06-13 | Cirrus Logic, Inc. | System and method for semiconductor device random telegraph sequence noise testing |
Family Cites Families (19)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US4430897A (en) * | 1981-05-14 | 1984-02-14 | The Board Of Trustees Of The Leland Stanford University | Acoustic microscope and method |
| GB2269465A (en) * | 1992-08-06 | 1994-02-09 | Inductotherm Europ | Induction heating |
| US6034978A (en) * | 1999-05-12 | 2000-03-07 | Cymer, Inc. | Gas discharge laser with gas temperature control |
| US6549022B1 (en) | 2000-06-02 | 2003-04-15 | Sandia Corporation | Apparatus and method for analyzing functional failures in integrated circuits |
| JP2004177350A (en) * | 2002-11-28 | 2004-06-24 | Denso Corp | Radar equipment for vehicles |
| US6967491B2 (en) * | 2003-07-11 | 2005-11-22 | Credence Systems Corporation | Spatial and temporal selective laser assisted fault localization |
| JP3966301B2 (en) * | 2004-03-25 | 2007-08-29 | 株式会社デンソー | Radar equipment for vehicles |
| US20090216494A1 (en) * | 2006-01-23 | 2009-08-27 | Stadler Andrew D | Network Laser System with Remote Diagnostics |
| US7830165B2 (en) * | 2006-03-31 | 2010-11-09 | Integrated Device Technology, Inc. | System and method for detecting single event latchup in integrated circuits |
| JP2009115764A (en) | 2007-11-09 | 2009-05-28 | Toshiba Corp | Semiconductor inspection apparatus and semiconductor inspection method using the same |
| US8907691B2 (en) | 2009-06-24 | 2014-12-09 | Applied Micro Circuits Corporation | Integrated circuit thermally induced noise analysis |
| US8797052B2 (en) | 2009-11-14 | 2014-08-05 | James B. Colvin | System and method for gradient thermal analysis by induced stimulus |
| JP2012037310A (en) | 2010-08-05 | 2012-02-23 | Renesas Electronics Corp | Failure analyzer and failure analysis method of semiconductor integrated circuit |
| US8937272B2 (en) * | 2011-12-12 | 2015-01-20 | Aptina Imaging Corporation | Vertical JFET source follower for small pixel CMOS image sensors |
| US9304741B2 (en) * | 2013-04-22 | 2016-04-05 | Omnivision Technologies, Inc. | Apparatus, method and system for random number generation |
| US9564380B2 (en) * | 2014-08-26 | 2017-02-07 | Sandisk Technologies Llc | Marker pattern for enhanced failure analysis resolution |
| WO2016069802A1 (en) * | 2014-10-28 | 2016-05-06 | Advanced Charging Technologies, LLC | Electrical circuit for delivering power to consumer electronic devices |
| TW201809712A (en) | 2014-10-29 | 2018-03-16 | 因諾帝歐股份有限公司 | Apparatus, method, and system for testing IC chip |
| US9608080B2 (en) * | 2015-03-05 | 2017-03-28 | International Business Machines Corporation | Method and structure to reduce parasitic capacitance in raised source/drain silicon-on-insulator devices |
-
2016
- 2016-06-07 US US15/175,871 patent/US9723578B2/en active Active
- 2016-06-08 EP EP16730301.5A patent/EP3308180A1/en not_active Withdrawn
- 2016-06-08 KR KR1020187000497A patent/KR102291679B1/en active Active
- 2016-06-08 CN CN201680046733.6A patent/CN107923940A/en active Pending
- 2016-06-08 WO PCT/EP2016/063072 patent/WO2016198475A1/en not_active Ceased
Also Published As
| Publication number | Publication date |
|---|---|
| KR20180016515A (en) | 2018-02-14 |
| KR102291679B1 (en) | 2021-08-23 |
| WO2016198475A1 (en) | 2016-12-15 |
| US20160366656A1 (en) | 2016-12-15 |
| US9723578B2 (en) | 2017-08-01 |
| CN107923940A (en) | 2018-04-17 |
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